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Many gamma-ray sources are unidentified and may be pulsars, but establishing ... search did not find any previously unknown gamma-ray pulsars in EGRET data. ... – PowerPoint PPT presentation

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Title: John%20Rice


1
Detecting Periodicity in Point Processes
  • John Rice
  • University of California, Berkeley
  • All animals act as if they can make decisions.
    (I. J. Good)
  • Joint work with Peter Bickel and Bas Kleijn.
    Thanks to Seth Digel, Patrick Nolan and Tom
    Loredo

2
Outline
Introduction and motivation A family of score
tests Assessing significance in a blind
search The need for empirical comparisons
3
Motivation
Many gamma-ray sources are unidentified and may
be pulsars, but establishing that these sources
are periodic is difficult. Might only collect
1500 photons during a 10 day period.
4
Difficulties
  • Frequency unknown
  • Spins down
  • Large search space
  • Glitches
  • Celestial foreground

Computational demands for a blind search are very
substantial. A heroic search did not find any
previously unknown gamma-ray pulsars in EGRET
data. (Chandler et al, 2001).
5
Detection problem
6
Unpleasant fact There is no optimal test.
A detection algorithm optimal for one function
will not be optimal for another function. No
matter how clever you are, no matter how rich the
dictionary from which you adaptively compose a
detection statistic, no matter how multilayered
your hierarchical prior, your procedure will not
be globally optimal. The pulse profile ?(t) is
an infinite dimensional object. Any test can
achieve high asymptotic power against local
alternatives for at most a finite number of
directions. In other words, associated with any
particular test is a finite dimensional
collection of targets and it is only for such
targets that it is highly sensitive. Consequence
You have to be a closet Bayesian and choose
directions a priori.
Lehman Romano. Testing Statistical Hypotheses.
Chapt 14
7
Specifying a target
8
Likelihood function and score test
  • Let the point spread function be w(ze). The
    likelihood given times (t), energies (e), and
    locations (z) of photons

where wj w(zj ej).. A score test (Rao test)
is formed by differentiating the log likelihood
with respect to ? and evaluating the derivative
at ? 0
Neglible if period ltlt T
Unlike a generalized ratio test, a Rao test does
not require fitting parameters under the
alternative, but only under the null hypothesis.
9
Phase invariant statistic
  • Square and integrate out phase. Neglecting the
    second term
  • Apart from psf-weighting was proposed by Beran as
    locally most powerful invariant test in the
    direction ?( ) at frequency f. Truncating at n1
    gives Rayleigh test. Truncating at nM gives
    ZM2. Particular choice of coefficients gives
    Watsons test (invariant form of Cramer-von
    Mises).

Mardia (1972). Statistics of Directional Data
10
Relationship to tests based on density estimation
  • In the unweighted case the test statistic can be
    expressed as
  • A continuous version of a chi-square goodness of
    fit test using kernel density estimate rather
    than binning. But note that a kernel for density
    estimation is usually taken to be sharply peaked
    and thus have substantial high frequency content!
    Such a choice of ?( ) will not match low
    frequency targets.

Kernel density estimate
11
Power
  • Let
  • And suppose the signal is
  • and
  • Then

12
Tradeoffs
  • The n-th harmonic will only contribute to the
    power if ?n is substantial and if n? is small.
    That is, inclusion of harmonics is only helpful
    if the signal contains substantial power in those
    harmonics and if sampling is fine, n??lt 1
    compared to the spacing of the Fourier
    frequencies, 1/T otherwise the cost in variance
    of including higher harmonics may more than
    offset potential gains. Viewed from this
    perspective, tests based on density estimation
    with a small bandwidth are not attractive unless
    the light curve has substantial high frequency
    components and the target frequency is very close
    to the actual frequency.

13
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14
Integration versus discretization
  • Rather than fine discretization of frequency,
    consider integrating the test statistic over a
    frequency band using a symmetric probability
    density g(f).

15
  • Requires a number of operations quadratic in the
    number of photons. However the quadratic form
    can be diagonalized in an eigenfunction
    expansion, resulting in a number of operations
    linear in the number of photons.
  • (In the case that g() is uniform, the
    eigenfunctions are the prolate spheroidal wave
    functions.) Then
  • Power is still lost in high frequencies unless
    the support of g is small.
  • This procedure can be extended to integrate over
    tiles in the plane when

MultiTaper
16
Example Vela
17
Assessing significance
  • At a single frequency, significance can be
    assessed easily through simulation. In a
    broadband blind search this is not feasible and
    furthermore one may feel nervous in using the
    traditional chi-square approximations in the
    extreme tail (it can be shown that the limiting
    null distribution of the integrated test
    statistic is that of a weighted sum of chi-square
    random variables). We are thus investigating the
    use of classical extreme value theory in
    conjunction with affordable simulation.

18
Gumbel Approximation
19
Example
20
Tail Approximations
According to this approximation, in order for a
Bonferonni corrected p-value to be less than
0.01, a test statistic of about 11 standard
deviations or more would be required.
21
log- log F(t) versus t
22
Need for theoretical and empirical comparisons
  • Since no procedure is a priori optimal,
    comparisons are needed.
  • Suppose we are considering a testing procedure
    such as that we have described and two Bayesian
    procedures
  • A Gregory-Loredo procedure based on a step
    function model for phased light curve
  • A prior on Fourier coefficients, eg independent
    mean zero Gaussian with decreasing variance
  • Also note that within each of these two, the
    particular prior is important. Even in
    traditional low-dimensional models, the Bayes
    factor is sensitive to the prior on model
    parameters, in contrast to its small effect in
    estimation.
  • Kass Raftery (1995). JASA. p. 773-

23
Example
  • We run the procedure discussed earlier with
  • We also use a Bayesian procedure
  • The signal has
  • How do the detection procedures compare?

24
  • To compare a suite of frequentist and Bayesian
    procedures, we would like to like to understand
    the behavior of the Bayes factors if there is no
    signal and if there is a signal. (Box suggested
    that statistical models should be Bayesian but
    should be tested using sampling theory). Theory
    for the Bayesian models above?
  • It might be possible to convert p-values to Bayes
    factors.
  • It might be possible to evaluate posterior
    probabilities of all the competing models and
    perform composite inference (would involve
    massive computing).
  • Inference is constrained by computation.
  • Touchstone blind comparisons on test signals.
    We understand that GLAST will be making such
    comparisons.

Box (1981). In Bayesian Statistics Valencia
I Good (1992) JASA
25
Conclusion
Problems are daunting, but with imagination, some
theory, and a lot of computing power, there is
hope for progress.
NERSC's IBM SP, Seaborg, has 6,080 CPUs .
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